METHOD OF SEPARATION AND ANALYSIS

Abstract: Particles are subjected to travelling wave field migration (TWFM) to migrate the particles over an array of microelectrodes. Altered particles are produced by treating original particles in such a way so as to alter their TWFM characteristics and the altered TWFM characteristics are employed for analysis and/or separation of the altered particles. The particles may be cells, bacteria, viruses, biomolecules or plastics microspheres. They may be altered by binding to a ligand such as a metal microparticle via a selective linking moiety such as an antibody/antigen or oligo-nucleic acid, or by physical or chemical treatments.

Description: The present invention relates to analytical methods based upon the observation of the migration of particles in response to an electric field. By way of background, particles can be manipulated by subjecting them to travelling electric fields. Such travelling fields are produced by applying appropriate voltages to microelectrode arrays of suitable design. The microelectrodes have the geometrical form of parallel bars, which may be interrupted by spaces to form channels, as shown in figure 1 and may be fabricated using standard metal sputtering and photolithographic techniques as described by Price, Burt and Pethig, Biochemica et Biophysica, Vol.964, pp.221-230. Travelling electric fields are generated by applying voltages of suitable frequency and phases to the electrodes as described in a paper, title "Separation of small particles suspended in liquid by nonuniform travelling field", by Masuda, Washizu and Iwadare, IEEE Transactions on Industry Applications, Vol.IA-23, pp.474-480. Masuda and his coworkers describe how a series of parallel electrodes (with no channels) supporting a travelling electric field can, in principle, be used to separate particles according to their electrical charge and size (weight). Masuda et al have not however described a practical demonstration of such a particle separation method. In a paper entitled "Travelling-wave dielectrophoresis of microparticles" by Hagedorn, Fuhr, Müller and Gimsa (Electrophoresis, Vol.13, pp.49-54) a method is shown for moving dielectric particles, like living cells and artificial objects of microscopic dimensions, over microelectrode structures and in channels bounded by the electrodes. The travelling field was generated by applying voltages of the same frequency to each electrode, with a 90° phase shift between neighbouring electrodes. In "Electrokinetic behaviour of colloidal particles in travelling electric fields: Studies using Yeast cells" by Y Huang, X-B Wang and R Pethig J. Phys. D. Appl. Phys. 26 1993 1528-1535, an analysis supported by experiment is made of the "travelling-wave dielectrophoresis" (TWD) effect described by Hagedorn et al (paper cited above). The phenomenological equation µ = - 2π ε m r 2 3λη A 2 ( O ) Im [ f (ε * p ,ε * m )] is developed by Huang et al, to show that the TWD velocity is a function of the square of the particle radius (r), the square of the electric field strength (A(0)), the periodic length of the travelling field (λ), medium viscosity (η) and the imaginary part of the Clausius-Mossotti factor f(ε p *,ε m *) defining the dielectric properties of the particle and the suspending medium in terms of their respective complex permittivities ε p * and ε m *. This equation provides, for the first time, a practical guide for the design of travelling wave electrode systems for the manipulation and separation of particles. Although the phenomenon in question is usually termed "travelling wave dielectrophoresis", we have now demonstrated that this is something of a misnomer as the force which acts on the particles to produce translational movement is not the dielectrophoresis force but rather that which acts in electrorotation. This force is related to the imaginary component of the polarisability of the particle within its surrounding medium. However, as is discussed in more detail below, particle migration only occurs for travelling wave frequencies which produce negative dielectrophoretic forces on the particle. (Dielectrophoretic forces are related to the real component of the polarisability of the particle within its surrounding medium.) These forces are responsible for lifting the particle away from the electrodes and the channel between the electrodes. We accordingly prefer to refer to the phenomenon called previously "travelling wave dielectrophoresis" by the name "travelling wave field migration" (TWFM). We have established that to obtain TWFM, two separate criteria have to be met. First, a frequency must be selected at which the dielectrophoresis force acting on the particles is negative, ie such as to repel the particles from the electrodes. This, we have found requires the real component of the dipole moment induced in the particles to be negative. Second, the frequency selected has to be such that the imaginary component of the dipole moment induced in the particles is non-zero (whether positive or negative) to produce a force displacing the particles along the array of electrodes. WO-A-92/07657 discloses arrays of electrodes for use in producing travelling wave migration of particles. EP-A-718038 (published after the priority date of this case) discloses further arrangements of electrodes, including in Figure 4 an arrangement in which the spacing between subsequent electrodes in a "ladder" of electrodes progressively increases in the direction of particle migration. The present invention provides a method of particle transport comprising subjecting particles to travelling wave field migration in a channel defined between two rows of electrodes separated by said channel, wherein the width of the channel progressively decreases in the direction of the particle migration. The method may be applied where the particles are of sufficient size to be resolved by the use of light-microscope or where the particles are too small to be resolved by the use of a light micro-scope. The particles may comprise a complex formed btween an original particle and a ligand. The invention includes a method of particle transport comprising subjecting particles to travelling wave field migration in a channel defined between two rows of electrodes separated by said channel, wherein the spacing between successive ones of said electrodes in each said row progressively decreases in the direction of particle migration and wherein the width of the channel progressively decreases in the direction of particle migration. The invention also includes an electrode array for use in TWFM comprising a first row of electrodes, the spacing between successive ones of which electrodes in said first row progressively decreases, and wherein the array comprises a second row of electrodes, the spacing between successive ones of which electrodes in said second row progressively decreases, said first and second rows being arranged on opposite sides of a channel spacing separating said rows, the width of which channel progressively decreases as the spacing between successive electrodes progressively decreases. The method of particle transport described herein may be used in methods of separating particles as described in parent European Patent EP-B-0680380 including methods of separation comprising treating a particle to form an altered particle, which altered particle has TWFM properties distinct from those of the original particle, and producing translational movement of said altered particle by TWFM using conditions under which the movement of the altered particle is different from that which would be obtained using the original particle under identical conditions. The particle may be of a size to be visible using a light microscope (a microscopic particle) or may be smaller (a sub-microscopic particle) and may be detected using labels such as luminescent, fluorescent and electromagnetic radiation absorbent labels. Examples of the former type of particle include mammalian cells, plant cells, yeast cells, plastics micro-beads, chromosomes undergoing meiosis and mitosis and oocytes, eg. of Cryptosporidium. Examples of the second type would include bacterial cells, viruses, DNA or RNA molecules, proteins, other biomolecules, and chromosomes. The nature of the treatment used to convert the original particle into an altered particle can vary widely according to the nature of the particle. The treatment may involve forming a complex between the particle and a ligand. In some cases, the complex may involve a linking moiety connecting the particle and the ligand. The complex may further include a label connected to said ligand, optionally via a second linking moiety. The complex may involve numerous ligands bound to the particle. The choice of linking moiety will obviously depend on the nature of the particle and the ligand. For instance if one wishes to capture a nucleic acid species (the ligand) on a plastics micro-sphere (the particle), the linking moiety will normally be chosen to be a nucleic acid or nucleic acid analogue oligomer having a sequence complementary to that of the ligand or a part thereof. The linking moiety may be bound first to the particle and may then be a species having an affinity for the ligand. Preferably, said affinity for the ligand is a selective affinity such that the formation of the complex between the particle and the ligand is selective and provides at least a degree of identification of the ligand. Preferably, said affinity is highly specific and accordingly the said linking moiety bound to the particle which provides the selective affinity for the ligand may be an antibody or an antibody fragment having antibody activity, an antigen, a nucleic acid probe or a nucleic acid analogue probe having selective affinity for complementary nucleic acid sequences, or avidin or an avidin-like molecule such as strept-avidin. Antibodies and antibody fragments having antibody properties are particularly preferred. There are known techniques suitable for coating antibodies on to the surface of particles such as plastics micro-beads which are well known to those skilled in the art. Antibody coated particles are capable of recognising and binding corresponding antigens which may be presented on micro-organism cells or some other ligand. Methods are also known for binding oligo-nucleic acid probes to such micro-beads. Suitable techniques are by way of example described in PCT Application No. GB92/01526. Where the linking moiety is a nucleic acid probe or a nucleic acid analogue probe, the resulting particle will of course be suitable for recognising and binding complementary nucleic acid sequences. The ligand may be chosen to increase the visibility of the particle or otherwise improve its detectability as well as to alter its TWFM characteristics. For instance antibodies bearing fluorophores or chromaphores may be bound to the particle so that the complex so formed can be distinguished from the starting particle by TWFM and detected by fluorescence or colour. The label may be bound to said ligand either before, simultaneously with, or after the formation of the complex between the ligand and the particle. The label may comprise a second linking moiety carried by said label. Once again, it is preferred that the affinity for the ligand possessed by the second linking moiety is selective, preferably highly specific and the second linking moiety may also be an antibody, an antibody fragment having antibody activity, an antigen, a nucleic acid probe, a nucleic acid analogue probe, avidin or an avidin-like molecule. The use of a label of this nature may be desired to aid ready detection of the complex and/or where a complex between the particle and the ligand does not in itself possess sufficiently distinctive TWFM properties, thus the TWFM may be further altered by the inclusion in the complex of the label. To this end, the label may be a fluorophore or chromaphore, or a micro-organism, a metal particle, a polymer bead or a magnetic particle. For use in connection with TWFM measurements, the label preferably has dielectric properties and is capable of acquiring a significant surface charge. A particularly preferred material is colloidal gold which is easily bound to antibodies (as said second species) to form a label. Antibodies bound to colloidal gold are commercially available and methods for binding antibodies to colloidal gold are for instance described in Geohegan W.D. et al (1978) Immunol. Comm 7 pl. Other metal particles however may be employed, eg silver particles and iron particles. The use of a label of the kind described above may be preferred even where a complex between the ligand and a particle possesses sufficiently distinctive TWFM properties to enable the formation of such a complex to be observed. A higher level of specificity may in certain cases be obtained by the use of a label in such a complex. Thus for instance, one may wish to distinguish a micro-organism expressing an antigen A from a micro-organism expressing antigens A and B. This may be accomplished by the use of micro-particles having as a linking moiety an antibody to A and a label having as it's moiety an antibody to B. The difference in the velocities of the labelled complex (between the micro-particle, the micro-organism and the label) and the unlabelled complex (between the micro-particle and the micro-organism) can be observed, and used to distinguish micro-organisms expressing antigen A only, from those expressing A and B. The label may include a magnetic particle so that the label can be attracted to a magnet so as to concentrate complexes containing said label for easier observation. In some cases it may be possible to attract labelled complexes to a magnet and to wash away unlabelled particles so as to eliminate the background of particles bearing linking moieties but no ligand/label which would normally be present. Suitable magnetic labels for this purpose will include iron micro-particles bearing linking moieties such as antibodies. Such antibody coated iron particles are commercially available. Labels for both cells and smaller particles can include fluorescent markers eg FITC or rhodamine, chromophores, luminescent markers or enzyme molecules which can generate a detectable signal. Examples of the latter include luciferases and alkaline phosphatase. These markers may be detected using spectroscopic techniques well known to those skilled in the art. The label could be bound to the ligand either before, simultaneously with, or after the formation of the complex between the ligand and the particle. In the case of cell transfection, the cells may co-express a marker with the gene product. For example, the gene for firefly or bacterial luciferase may be co-transfected into the cells enabling the transfected cells to be visualised by a luminescent signal. The alteration of the original particle need not involve the formation of a complex. For instance, the TWFM characteristics of a cell may be altered by heating or by treatment with a reagent which alters the porosity of the cell membrane. Accordingly, the alteration may be in the particle itself rather than or in addition to a change due to the physical presence of a ligand in a complex. Both effects may be present in combination. A ligand forming a complex with a particle may exert a physical effect on the TWFM properties and also by interaction with the particle bring about a change in the intrinsic TWFM properties of the particle. The invention includes methods of particle transport carried out for analytical purposes and also such methods carried out for preparative or other purposes. The methods according to the invention may be employed in a wide variety of analytical applications including separation and analysis of samples containing cells for example, bacterial, mammalian, yeast, and insect cells or virus particles, and, biological macromolecules. Current methods of separating cells, for example flow cell cytometry, require expensive instrumentation, skilled operators and significant laboratory resources. The techniques also have limitations when there are many different cell populations to be separated and when the cells of interest represent less than a few percent of the total. For separation and analysis of modified biological molecules, or complexes between biological macromolecules, employed techniques include electrophoresis and chromatographic separation using gel-filtration or affinity chromatography. Although these, in some cases, provide adequate separation, for many applications they can be time consuming and have limited resolution. In addition, use of these methods can affect the equilibrium between biological complexes. For example, gel-filtration results in a significant dilution of the sample. Methods described hereafter according to the present invention allow some or all of these drawbacks to be addressed. Where in an analytical method according to the invention a complex between the particle and a ligand is produced, the ligand need not itself be the species to establish the presence, nature or quantity of which is the ultimate purpose of the analysis. Thus, the ligand may be a reagent in the analysis and the species of interest in the analysis may be another component of the complex, eg the linking moiety or the particle itself. Where a particle is altered by treatment with a reagent, it may be the particle or the reagent which is essentially to be studied. The process of TWFM described previously has been carried out using an array of linear, parallel electrodes subjected to phased electric fields normally such that every fourth electrode along the TWFM path is in phase. This periodicity defines the effective wave length of the travelling wave field produced. We have established that this wave length is optimally about ten times the average diameter of the particle to be moved under TWFM, eg from 5 to 20 times or more preferably 8 to 12 times said average diameter. For particles which are not roughly circular, it is the length in the direction transverse to TWFM movement which is of significance. The electrodes for use in this invention may be formed, depending on the dimensions required, using any of the standard techniques for patterning and manufacturing microscopic structures. For example the electrodes can be produced by: screen printing; deposition of electrode material (eg by electroplating or sputter deposition) followed by one of the following patterning techniques: direct writing using an electron beam followed by etching (eg wet chemical etching, dry plasma etching or focused ion beam etching); writing by exposure through a photolithographically generated mask followed by etching - the mask may be generated for example by visible, ultra violet, X-ray or electron beam lithography; excimer laser ablation; patterning followed by deposition of the electrode material (as in the X-ray LIGA process). The invention will be further described and illustrated by the following description of apparatus and methodology with reference to the accompanying drawings in which: Figure 1 shows an electrode array in which the electrode spacing varies across the array; Figure 2 shows a further modified electrode array in which the electrode spcing varies both across and along the array. Examples of electrode designs for achieving separation effects are shown in Figures 1 and 2. In Figure 1, the array of electrodes is constituted by two parallel rows of electrodes, each electrode being rectangular and elongate transverse to the direction of extension of the rows. The two rows are separated by a gap the separation between each pair of electrodes in each row is the same. The electrodes are thin metal film electrodes on an insulating substrate, suitably gold electrodes printed on a glass slide. The separation between the rows decreases progressively. The pitch between groups of four electrodes in each row is 80µm. A useful rule is that generally the said pitch defining the wave length of the travelling wave should be from 5 to 20 times the size of the particle, eg 8 to 12 times, most preferably 10 times. The response of particles exposed to a travelling wave field of the kind described below can be varied. Particles can be collected on the electrodes, they can be induced to spin and they can be caused to travel along the gap between the rows or over the electrode rows. This travelling type of movement is TWFM. The type of motion produced depends upon the nature of the particle, the suspending medium, the electrode spacing and the field frequency. In Figure 2, the periodic length between electrodes varies, so as to bring into effect the parameter λ in the above equation. For example, a travelling wave moving from the top to bottom electrodes, will accelerate a particle moving upwards under TWFM. This may be used for example to produce more uniform resolution along the TWFM path, counteracting a natural tendency for resolution to increase with distance travelled. In Figure 1 and Figure 2 the channel width also varies, and this brings into play the variation of the field A(0) of the above equation. A particle moving under TWFM will be accelerated as a result of the field increasing as the channel width decreases. Thus, two particles of different size but otherwise similar physico-chemical properties will be spatially separated as they move along the channel. Particles of different dielectric properties could be suspended in suitable medium such that the factor Im[f(ε p *,ε m *)] in the above equation has a different sign for each particle. The particles would then set the frequency of the sine wave outputs and the peak to peak voltage of them. In use, the image appearing on the display of the apparatus shows a number of beads within the field of the microscope migrating sufficiently slowly that the rate of migration within a period such as 30 seconds can be determined directly by an observer looking at each bead in turn. Whilst apparatus described above is sufficient to produce useful results as demonstrated by the specific examples given below, it is generally preferable that migration speed measurements be carried out on more beads than a human observer could reasonably deal with directly. For this purpose, it will be desirable to use image processing techniques to detect and measure the migration of the beads in the apparatus. From the CCD camera attachment, one may derive images of a field of view containing a number of migration beads. A series of such images, or frames, may be captured by frames-grabber circuitry in a computer and the series of the images may be analysed by image processing software. Thus, a thresholding process may be used for example to convert the grey scale image produced by the camera into a binary image. A separate thresholding operation is performed to identify any areas of the image which are considered too dark, these areas being removed from the binary image of the beads. The remaining shapes in the image may be separated from the rest of the image and subjected to a test of one of more characteristic properties, such as area, to select those which are likely to represent beads. The centre of mass may then be determined for each qualifying shape. The positions of the centres may be compared between the successive frames in order that each bead in one frame may be located in the next. Once a bead has been located in two frames, the difference in the position of the bead will give directly the migration distance from which its migration rate may be calculated and averaged over several pairs of frames. By such automated techniques the migration speeds of all of the beads within the field of view at any moment may be measured and a statistical picture of the migration characteristics of the beads may be developed, optionally using a number of field migration frequencies. Other image processing techniques may also be used to identify the position of particles and to determine their movement, for example correlation, edge detection, or morphological techniques or images subtration. Neural networks may also be used to identify particles. It is not always necessary to use an imaging detector of the type described above to determine particle velocities. Alternative detection configurations include: light scatter detectors, as in a flow cytometer; standard fluorescence detection arrangements; luminescence detection using CCDs or other detectors; single or multi-element optical spectroscopic measurements; refractive index modulation detection (eg by phase contrast techniques); detection by acoustic impedance measurement (which is related to particle mass) using surface or bulk acoustic sensors; electrical impedance, capacitance, or inductance. The apparatus may be further modified by the inclusion of a magnet, suitably an electro-magnet, positioned to draw any magnetic beads in the sample into the field of view of the microscope. The magnet would then be removed or turned off whilst the migration characteristics of the beads were measured. Alternatively, the particles may be manipulated into position by dielectrophoresis or electrophoresis. A micro-particle may comprise a plastics bead having bound to it as a linking moiety one or more antibody molecules. Normally in reality the plastics beads will be coated with a multitude of antibody molecules. The micro-particles may be exposed to micro-organism cells bearing surface antigens reactive with the bound antibody to form a complex between the micro-particle and the cell. The micro-organism cells may for instance be E. coli or coliforms present in water or pathogenic micro-organisms present in foodstuffs such as listeria or salmonella. It has been found that the rate of migration of such micro-particle/micro-organism cell complexes under suitably chosen conditions is distinguishable from the migration rates obtained using the micro-particles alone and furthermore that the migration rates obtained for complexes between micro-particles and viable micro-organism cells can be distinguished from those obtained between micro-particles and similar non-viable cells. A ternary complex may be produced between a micro-particle, an antigen and a label comprising a labelling moiety and a second antibody which may be the same as or different from the antibody. A ternary complex of this type may be employed where the antigen is too small or lacking in dielectric properties sufficiently to affect the TWFM properties of the micro-particle or where it is desired to obtain a higher level of specificity through the use of two different antibodies in a single analysis. The antigen may for instance be a toxin present as a contaminant in a foodstuff. The invention includes methods of detecting nucleic acids and in particular nucleic acid sequences produced as products of amplification procedures such as PCR, LCR and 3SR techniques. Known methods of detecting nucleic acid amplification procedure products rely upon them undergoing some form of purification and/or separation procedure before they are analysed. One commonly used method involves the analysis of the products by agarose gel electrophoresis. This separates the amplified DNA fragments and any remaining oligonucleotide primers on the basis of size. Separating products on the basis of size alone does not enable one to distinguish between PCR products of the required base sequence and an amplified contaminant of approximately the same length. In order to further identify PCR products, the gel electrophoresis may be taken one step further by subjecting its product to the Southern blotting technique in which the separated fragments are transferred from the gel to a membrane in direct correspondence to their relative positions on the gel. They are then probed with a labelled single stranded DNA probe with a base sequence complementary to the sequence of interest. The label used for the probe is usually biotin or a radio-isotope such as 32 P. Southern blotting is relatively laborious and requires a moderate level of laboratory skill as well as laboratory equipment and facilities. It is not suited for use in rapid screening of a large number of samples or the screening of samples outside the laboratory. The method of dot blotting in which the agarose gel separation step of Southern blotting is omitted is somewhat quicker but basically suffers from the same disadvantages as Southern blotting. In a method according to the present invention a microparticle may include an oligonucleotide or synthetic oligonucleotide analogue as a capture probe (linking moiety) bound to the surface of a polymer bead and having a sequence complementary to that of an expected amplification procedure product. A label comprising an TWFM labelling moiety as described above bound to a second oligonucleotide or oligonucleotide analogue sequence complementary to a second region of the ligand nucleic acid sequence is employed. The micro-particles and the label may be added to the product of the amplification reaction before or after any working up of the reaction mixture to separate the amplification products. The TWFM properties of the micro-particle/amplification product/label ternary complex may then be observed and distinguished from those of the micro-particles alone. In a variant on this procedure one of the primers used in the amplification procedure is labelled with a suitable TWFM labelling moiety which thereby becomes covalently incorporated into the nucleic acid product of the amplification procedure. A binary complex is then produced between a micro-particle bearing a capture probe 26 and the amplification product and the TWFM properties of the complex are observed. The ligand nucleic acid may be a chromosome (complex nucleic acid) and the micro-particle may have discrete dielectric properties eg is metallic (gold) etc. This is particularly useful for the separation of human (and other species) chromosomes where different chromosomes may have similar sizes, and dielectric properties. Technologies such as flow cytometry are currently used to sort chromosomes on a size basis, and are thus incapable of discriminating chromosomes of similar sizes. In the case of humans, chromosomes 9-12 inclusive can not readily be separated by flow cytometry due to their similar size. According to our approach if these chromosomes are pre-labelled with a 'dielectric' marker they can be separated on the basis of their dielectric properties. In practice this is achieved by partially denaturing the chromosomal DNA (by for example heat, chemical treatment, or electrical treatment), and subsequently hybridising a complementary (to a defined nucleic acid sequence) nucleic acid probe. The nucleic acid probe may preferably consist of at least 15 nucleotides, and may itself be pre-labelled with an entity which has an affinity for a binding agent. For example, but not exclusively, the label may be 'biotin' which can be incorporated into a nucleotide, or added to the terminal region of the probe sequence. The binding agent may be for example, an antibody which has specificity for the label, or alternatively a protein/enzyme etc which has an affinity for the label of choice. The binding agent may in turn be bound to a micro-particle which could as both a dielectric amplifier (by amplifying additional dielectric properties) and/or an aid to detection of the chromosomes of choice. Following the 'dielectric labelling' of the ligand chromosome it can then be separated from the other chromosomes on the basis of different dielectric properties. Thus it is possible to see that the selective separation and identification of chromosomes could be achieved using the method described above. This has practical application in clinical diagnostics where, identification and characterisation of chromosome alterations, eg re-arrangements/dilutions, insertion of foreign DNA eg viral DNA is important. Alternatively, the chromosome may be the particle and it may be treated by hybridisation thereto of a nucleic acid probe bearing a label (the ligand) which alters the TWFM characteristics of the chromosome and optimally which also aids its detection, eg a fluorescent marker. Further details of uses of the electrode arrays described herein are to be found in EP-A-0680380. Examples of analyses and separations possible using the techniques of the invention are as follows. A double stranded DNA molecule having attached to it a protein such as a transcription factor (altered particle) may be separated from DNA lacking the protein by selecting conditions under which only the altered particle migrates and the protein may then be cleaved off isolated, sequenced and studied. In a variant of the above the protein-DNA complex may be separated from similar protein-DNA complexes to which an additional protein has bound (altered particle). A cell having on its surface a receptor for a ligand such as an antibody, growth factor, neurotransmitter or other biochemical messenger may be separated from similar cells to which the appropriate ligand has bound. Cells which have been successfully transfected such that they express a new gene product, possibly located in the cell membrane, may be differentiated from the original form of cell. Cells to which a phage has bound may be differentiated from non-infected cells. Cells may have an oligonucleotide probe bound to a label such as a gold particle introduced into them to bind to complementary genomic DNA during cell division to separate dividing from non-dividing cells. Methods of detection used are not limited to microscopy. For instance, where the altered particle includes a dye or fluorescent marker, the presence of altered particles may be monitored by an appropriate spectrophotometer. The electrodes need not be arranged as a pair of linear "ladders". Instead each "ladder" of electrodes may be curved or otherwise non-linear. It may form a spiral or serpentine path.

Claims: A method of particle transport comprising subjecting particles to travelling wave field migration in a channel defined between two rows of electrodes separated by said channel, wherein the width of the channel progressively decreases in the direction of the particle migration. A method as claimed in Claim 1, wherein the particles are of sufficient size to be resolved by the use of light-microscope. A method as claimed in Claim 1, wherein the particles are too small to be resolved by the use of a light micro-scope. A method as claimed in Claim 1, wherein the particles comprise a complex formed between an original particle and a ligand. A method of particle transport comprising subjecting particles to travelling wave field migration in a channel defined between two rows of electrodes separated by said channel, wherein the spacing between successive ones of said electrodes in each said row progressively decreases in the direction of particle migration and wherein the width of the channel progressively decreases in the direction of particle migration. A method as claimed in Claim 5, wherein the particles are of sufficient size to be resolved by the use of a light-microscope. A method as claimed in Claim 5, wherein the particles are too small to be resolved by the use of a light-microscope. A method as claimed in any one of Claims 5 to 7, wherein the particles comprise a complex formed between an original particle and a ligand. An electrode array for use in TWFM comprising a first row of electrodes, the spacing between successive ones of which electrodes in said first row progressively decreases, and wherein the array comprises a second row of electrodes, the spacing between successive ones of which electrodes in said second row progressively decreases, said first and second rows being arranged on opposite sides of a channel spacing separating said rows, the width of which channel progressively decreases as the spacing between successive electrodes progressively decreases.

Inventors: HUANG YING, MACGREGOR ALASTAIR ROY, PARTON ADRIAN, PETHIG RONALD, POLLARD-KNIGHT DENISE VERA, WANG XIAO-BO, HUANG,YING, MACGREGOR,ALASTAIR ROY, PARTON,ADRIAN, PETHIG,RONALD, POLLARD-KNIGHT,DENISE VERA, WANG,XIAO-BO, Huang,Ying, c/o University of Texas, Wang,Xiao-Bo, c/o University of Texas
Applicants: SCIENT GENERICS LTD, SCIENTIFIC GENERICS LIMITED
Application year: 1994
Main classification: B03C5
IPC codes: G01N33, B03C5, C12N15, C12N13